Generalized curvature and the equations of D=11 supergravity

被引:9
|
作者
Bandos, IA [1 ]
de Azcárraga, JA
Picón, M
Varela, O
机构
[1] Univ Valencia, Dept Fis Teor, Burjassot 46100, Valencia, Spain
[2] UVEG, CSIC, IFIC, Burjassot 46100, Valencia, Spain
[3] NSC, Kharkov Inst Phys & Technol, Inst Theoret Phys, UA-61108 Kharkov, Ukraine
[4] Univ So Calif, Dept Phys & Astron, Los Angeles, CA 90089 USA
[5] Univ Michigan, Dept Phys, Randall Lab, Michigan Ctr Theoret Phys, Ann Arbor, MI 48109 USA
关键词
D O I
10.1016/j.physletb.2005.03.045
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
It is known that, for zero fermionic sector, psi(alpha)(mu) (x) = 0, the bosonic equations of Cremmer-Julia-Scherk eleven-dimensional supergravity can be collected in a compact expression, R-alpha b alpha(gamma) Gamma(b)(beta)(gamma) = 0, which is a condition on the curvature R-alpha(beta) of the generalized connection w. In this Letter we show that the equation R-bc alpha(gamma) Gamma(abc) (gamma beta) = 4i ((D psi)(bc) Gamma([abc))(beta)(psi d Gamma(d]))(alpha) where D is the covariant derivative for the generalized connection w, collects all the bosonic equations of D = 11 supergravity when the gravitino is nonvanishing, psi(alpha)(mu) (x) not equal 0. (c) 2005 Elsevier B.V. All rights reserved.
引用
收藏
页码:127 / 133
页数:7
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